9-strings Number of DOMs Vs Log(Npe) The high energy pole filter (NDOM>53) and the EHE criteria Npe>1.0e4 are plotted together |
9-strings Event rate as a functon of cos(theta-MC truth) Solid curve : Our "base cut" - Npe>200 NDOM >4 Dashed curve : High Energy pole filter - NDOM >53 Dotted curve : Our criteria - Npe >1.0e4 Left Panel: Weighted by Atmospheric muon flux(red) and GZK muon (blue) Right Panel: Unweighted. E^{-2}(red) and E^{-1}(blue) |
9-strings Event rate as a function of NPE (photoelectron sum) Solid curve : Our "base cut" - Npe>200 NDOM >4 Dashed curve : High Energy pole filter - NDOM >53 Dotted curve : Our criteria - Npe >1.0e4 Left Panel: Weighted by Atmospheric muon flux(red) and GZK muon (blue) Right Panel: Unweighted. E^{-2}(red) and E^{-1}(blue) |
80-strings Event rate as a function of NPE (photoelectron sum) After the "High Energy" filter NDOM > 80 Left Panel: Weighted by Atmospheric muon flux(red) and GZK muon (blue) tau (black) Right Panel: Integrated event rate (>Npe) adding both atm muon and the GZK's |
80-strings Event rate as a function of NDOM (Number of DOMs with reco pulse) After the "Unblinding NPE cut" Npe > 1.0e4 Left Panel: Weighted by Atmospheric muon flux(red) and GZK muon (blue) tau (black) Right Panel: Integrated event rate (>NDOM) adding both atm muon and the GZK's |
80-strings Event rate as a function of NDOM (Number of DOMs with reco pulse) Same as above, but with expanded scale. After the "Unblinding NPE cut" Npe > 1.0e4 Left Panel: Weighted by Atmospheric muon flux(red) and GZK muon (blue) tau (black) Right Panel: Integrated event rate (>NDOM) adding both atm muon and the GZK's |